2000
DOI: 10.1107/s010876730000996x
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The statistical kinematical theory of X-ray diffraction as applied to reciprocal-space mapping

Abstract: The statistical kinematical X-ray diffraction theory is developed to describe reciprocal-space maps (RSMs) from deformed crystals with defects of the structure. The general solutions for coherent and diffuse components of the scattered intensity in reciprocal space are derived. As an example, the explicit expressions for intensity distributions in the case of spherical defects and of a mosaic crystal were obtained. The theory takes into account the instrumental function of the triple-crystal diffractometer and… Show more

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Cited by 40 publications
(23 citation statements)
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“…The two expressions differ in that Eqn (3) contains the correlation volume instead of the correlation length [37,38,40]: This formula coincides with the expression for incoherent scattering intensity from onedimensionally deformed crystals in a double-axial recording scheme [31±33].…”
Section: Triple-axis X-ray Diffractometrymentioning
confidence: 62%
See 2 more Smart Citations
“…The two expressions differ in that Eqn (3) contains the correlation volume instead of the correlation length [37,38,40]: This formula coincides with the expression for incoherent scattering intensity from onedimensionally deformed crystals in a double-axial recording scheme [31±33].…”
Section: Triple-axis X-ray Diffractometrymentioning
confidence: 62%
“…is described by the intrinsic correlation function [28,38] gr; q exp  ih À dur q À dur Áà À f 2 r 1 À f 2 r : 5 The type of defects (shape, size, elastic strains, etc.)…”
Section: Triple-axis X-ray Diffractometrymentioning
confidence: 99%
See 1 more Smart Citation
“…¥Îâ ÐÇÍÑÕÑÓÞØ ÏÑAEÇÎÇÌ AEÇ×ÇÍÕÑÄ ÂÐÂÎËÕËÚÇÔÍÑÇ ÄÞÓÂÉÇÐËÇ ÔÑÃÔÕÄÇÐÐÑÌ ÍÑÓÓÇÎâÙËÑÐÐÑÌ ×ÖÐÍÙËË ÒÑÎÖ-ÚÇÐÑ Ä [38,39,47,48]. ²ÂÔÔÏÑÕÓÇÐËÇ AEË××ÖÊÐÑÅÑ ÓÂÔÔÇâ-ÐËâ Ä ÓÂÏÍÂØ ÕÓÈØÑÔÇÄÑÌ AEË×ÓÂÍÕÑÏÇÕÓËË ÕÓÇÃÖÇÕ ËÐÕÇ-ÅÓËÓÑÄÂÐËâ (4) ÒÑ ÒÇÓÇÏÇÐÐÑÌ q y .…”
Section: ³õâõëôõëúçôíââ õçñóëâ óçðõåçðñäôíñì Aeë×óâíùëëunclassified
“…²ÂÔÔÏÑÕÓÇÐËÇ AEË××ÖÊÐÑÅÑ ÓÂÔÔÇâ-ÐËâ Ä ÓÂÏÍÂØ ÕÓÈØÑÔÇÄÑÌ AEË×ÓÂÍÕÑÏÇÕÓËË ÕÓÇÃÖÇÕ ËÐÕÇ-ÅÓËÓÑÄÂÐËâ (4) ÒÑ ÒÇÓÇÏÇÐÐÑÌ q y . £ ÓÇÊÖÎßÕÂÕÇ ÍÑÓÓÇÎâ-ÙËÑÐÐÞÌ ÑÃÝÈÏ ÕÓÂÐÔ×ÑÓÏËÓÖÇÕÔâ Ä ÍÑÓÓÇÎâÙËÑÐÐÖá ÒÎÑÜÂAEß trY q x Y q z I ÀI dq y trY q [38,39]. £ ÔÎÖÚÂÇ ÑAEÐÑÓÑAEÐÑ ÓÂÔÒÓÇAEÇÎÈÐÐÞØ AEÇ×ÇÍÕÑÄ ÓÇÛÇÐËÇ AEÎâ ÍÑÓ-ÓÇÎâÙËÑÐÐÑÅÑ ÑÃÝÈÏ ÏÑÉÇÕ ÃÞÕß ÒÓÇAEÔÕÂÄÎÇÐÑ Ä ËÐÑÌ ×ÑÓÏÇ.…”
Section: ³õâõëôõëúçôíââ õçñóëâ óçðõåçðñäôíñì Aeë×óâíùëëunclassified